TW201710723A - Resin optical waveguide - Google Patents

Resin optical waveguide Download PDF

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Publication number
TW201710723A
TW201710723A TW105124663A TW105124663A TW201710723A TW 201710723 A TW201710723 A TW 201710723A TW 105124663 A TW105124663 A TW 105124663A TW 105124663 A TW105124663 A TW 105124663A TW 201710723 A TW201710723 A TW 201710723A
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Taiwan
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core
optical waveguide
refractive index
resin optical
cladding layer
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TW105124663A
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Chinese (zh)
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TWI693435B (en
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Seiki Ohara
Shotaro Takenobu
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Asahi Glass Co Ltd
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • G02B6/30Optical coupling means for use between fibre and thin-film device
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/122Basic optical elements, e.g. light-guiding paths
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/122Basic optical elements, e.g. light-guiding paths
    • G02B6/1221Basic optical elements, e.g. light-guiding paths made from organic materials
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/13Integrated optical circuits characterised by the manufacturing method
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B2006/12035Materials
    • G02B2006/12061Silicon
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B2006/12083Constructional arrangements
    • G02B2006/12088Monomode
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B2006/12083Constructional arrangements
    • G02B2006/12095Graded
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B2006/12133Functions
    • G02B2006/12147Coupler

Abstract

A resin optical waveguide is provided with a core, under-cladding having a lower refractive index than the core, and over-cladding. The resin optical waveguide is characterized in that a core exposure section in which the core is exposed and the over-cladding is not present is provided to one end side of the resin optical waveguide. The resin optical waveguide is also characterized by comprising a core vicinity area in which the part of the under-cladding corresponding to the core exposure section satisfies the conditions (1) and (2) indicated below. (1) The core vicinity area is an area within a distance x from the core and x is 5-20 [mu]m. (2) The core vicinity area has a refractive index distribution in which the refractive index on the interface side with the core is higher and the refractive index on the distal side with respect to the interface with the core is lower.

Description

樹脂光波導 Resin optical waveguide

本發明係關於一種樹脂光波導。 The present invention relates to a resin optical waveguide.

於非專利文獻1、2、或專利文獻1中提出有低損失且低成本地連接矽光波導與樹脂光波導之矽光子介面。本說明書中之所謂矽光波導係指於矽晶片上形成有作為(單模)光波導發揮功能之芯體包覆層構造者。 Non-patent documents 1, 2, and 1 are proposed to have a low-loss and low-cost connection of a photonic interface between a krypton waveguide and a resin optical waveguide. The term "boring waveguide" as used in the present specification means a structure in which a core cladding layer functioning as a (single mode) optical waveguide is formed on a germanium wafer.

圖3係表示此種矽光子介面之一構成例之立體圖,圖4為其側視圖。 Fig. 3 is a perspective view showing a configuration example of such a bismuth photo interface, and Fig. 4 is a side view thereof.

於圖3、4所示之樹脂光波導晶片300形成有1條或複數條樹脂光波導310。於樹脂光波導晶片300之一端側,樹脂光波導310與形成於矽光波導晶片200上之矽光波導(未圖示)連接。樹脂光波導晶片300之另一端側收容於連接器100內。 One or a plurality of resin optical waveguides 310 are formed in the resin optical waveguide wafer 300 shown in Figs. On one end side of the resin optical waveguide wafer 300, the resin optical waveguide 310 is connected to a pupil waveguide (not shown) formed on the calender waveguide wafer 200. The other end side of the resin optical waveguide wafer 300 is housed in the connector 100.

圖5係表示用於上述目的之樹脂光波導之一構成例之立體圖。 Fig. 5 is a perspective view showing a configuration example of one of the resin optical waveguides used for the above purpose.

圖5所示之樹脂光波導310係於芯體320之周圍配置有下包覆層330及上包覆層340。但是,於圖3、4中,與形成於矽光波導晶片200上之矽光波導(未圖示)連接之側之前端成為未配置上包覆層340而使芯體320露出於外部之芯體露出部350。 The resin optical waveguide 310 shown in FIG. 5 is provided with a lower cladding layer 330 and an upper cladding layer 340 around the core 320. However, in FIGS. 3 and 4, the front end connected to the pupil optical waveguide (not shown) formed on the neon waveguide wafer 200 is a core in which the upper cladding layer 340 is not disposed and the core 320 is exposed to the outside. The body exposed portion 350.

圖6係表示於圖3、4所示之矽光子介面中矽光波導210與樹脂光波導310之連接部之剖視圖,樹脂光波導310係圖5所示之樹脂光波導310。於圖6中,將矽光波導210與樹脂光波導310以樹脂光波導310之 芯體320面向矽光波導210之狀態使用環氧樹脂連接。 Fig. 6 is a cross-sectional view showing a connection portion between the pupil waveguide 210 and the resin optical waveguide 310 in the bismuth photo interface shown in Figs. 3 and 4, and the resin optical waveguide 310 is a resin optical waveguide 310 shown in Fig. 5. In FIG. 6, the pupil waveguide 210 and the resin optical waveguide 310 are in the resin optical waveguide 310. The state in which the core 320 faces the calender waveguide 210 is connected using an epoxy resin.

圖7係用以說明圖3、4所示之矽光子介面中之光之傳輸之模式圖。於圖7中,藉由絕熱耦合(adiabatic coupling),光自矽光波導210之芯體220向於樹脂光波導310前端露出之芯體320傳輸。繼而,光自樹脂光波導310之芯體320向光纖130之芯體140傳輸。 Figure 7 is a schematic view for explaining the transmission of light in the photonic interface shown in Figures 3 and 4. In FIG. 7, light is transmitted from the core 220 of the optical waveguide 210 to the core 320 exposed at the front end of the resin optical waveguide 310 by adiabatic coupling. Light is then transmitted from the core 320 of the resin optical waveguide 310 to the core 140 of the optical fiber 130.

[先前技術文獻] [Previous Technical Literature] [非專利文獻] [Non-patent literature]

非專利文獻1:Jie Shu, Ciyuan Qiu,Xuezhi Zhang,and Qianfan Xu,"Efficient coupler between chip-level and board-level optical waveguides", OPTICS LETTERS, Vol.36, No.18,pp3614-3616(2011) Non-Patent Document 1: Jie Shu, Ciyuan Qiu, Xuezhi Zhang, and Qianfan Xu, "Efficient coupler between chip-level and board-level optical waveguides", OPTICS LETTERS, Vol.36, No. 18, pp3614-3616 (2011)

非專利文獻2:Tymon Barwics,and Yoichi Taira,"Low-Cost Interfacing of Fibers to Nanophotonic Waveguides: Design for Fabrication and Assembly Toleranes", IEEE Photonics Journal, Vol.6, No.4,August,660818(2014) Non-Patent Document 2: Tymon Barwics, and Yoichi Taira, "Low-Cost Interfacing of Fibers to Nanophotonic Waveguides: Design for Fabrication and Assembly Toleranes", IEEE Photonics Journal, Vol.6, No. 4, August, 660818 (2014)

[專利文獻] [Patent Literature]

專利文獻1:美國專利第8,724,937號說明書 Patent Document 1: US Patent No. 8,724,937

圖5所示之樹脂光波導310係於安裝於圖3、4所示之矽光子介面之前,以與先前之樹脂光波導同樣之程序實施性能評價。於樹脂光波導之性能評價中,將單模光纖連接於樹脂光波導之前端。圖8係用以說明於圖5所示之樹脂光波導310之前端連接有單模光纖時之光之傳播之模式圖。於圖5所示之樹脂光波導310與單模光纖400之連接中存在如下問題:一部分光自樹脂光波導310之前端之芯體320露出之部位放射後未得以傳輸,又,產生連接損失。該連接損失於安裝於圖3、4所示之矽光子介面時並未產生,對於性能評價結果之可靠性降低。 The resin optical waveguide 310 shown in Fig. 5 was subjected to the same procedure as the previous resin optical waveguide before the mounting of the photonic interface shown in Figs. In the performance evaluation of the resin optical waveguide, a single mode fiber is connected to the front end of the resin optical waveguide. Fig. 8 is a schematic view for explaining the propagation of light when a single mode fiber is connected to the front end of the resin optical waveguide 310 shown in Fig. 5. In the connection between the resin optical waveguide 310 and the single-mode optical fiber 400 shown in FIG. 5, there is a problem that a part of the light is not transmitted after being radiated from the portion where the core 320 at the front end of the resin optical waveguide 310 is exposed, and connection loss occurs. This connection loss did not occur when mounted on the 矽 photonic interface shown in Figs. 3 and 4, and the reliability of the performance evaluation result was lowered.

本發明之目的在於,為了解決上述先前技術之問題,提供一種樹脂光波導,其適宜用於低損失且低成本地連接矽光波導與樹脂光波導之矽光子介面,且使用單模光纖之性能評價之可靠性較高。 SUMMARY OF THE INVENTION An object of the present invention is to provide a resin optical waveguide which is suitable for low-loss and low-cost connection of a germanium photonic interface of a krypton waveguide and a resin optical waveguide, and which uses the performance of a single mode fiber in order to solve the problems of the prior art described above. The reliability of the evaluation is high.

為了達成上述目的,本發明提供一種樹脂光波導,其特徵在於:其係具備芯體以及折射率低於該芯體之下包覆層及上包覆層者,於上述樹脂光波導之一端側,設置有不存在上包覆層而露出芯體之芯體露出部,上述下包覆層中相當於上述芯體露出部之部位具有滿足下述(1)、(2)之芯體附近區域:(1)上述芯體附近區域係自上述芯體之距離為x以內之區域,該x為5μm以上且20μm以下;(2)上述芯體附近區域具有如下折射率分佈:與上述芯體之界面側之折射率為高,相對於與該芯體之界面之遠位側之折射率變低。 In order to achieve the above object, the present invention provides a resin optical waveguide characterized in that it has a core body and a refractive index lower than a cladding layer and an upper cladding layer of the core body, on one end side of the resin optical waveguide. a core exposed portion in which the upper cladding layer is not present to expose the core, and a portion corresponding to the core exposed portion of the lower cladding layer has a region near the core (1) and (2) (1) The region in the vicinity of the core is a region within a distance of x from the core, and x is 5 μm or more and 20 μm or less; (2) the region near the core has a refractive index distribution: The refractive index at the interface side is high, and the refractive index on the far side of the interface with the core is lowered.

於本發明之樹脂光波導中,較佳為,上述芯體露出部之光傳輸方向之長度為100μm以上。 In the resin optical waveguide of the present invention, it is preferable that the length of the core exposed portion in the light transmission direction is 100 μm or more.

於本發明之樹脂光波導中,較佳為,上述芯體附近區域之折射率分佈為0.00004/μm以上。 In the resin optical waveguide of the present invention, it is preferable that the refractive index distribution in the vicinity of the core is 0.00004 / μm or more.

於本發明之樹脂光波導中,較佳為,上述芯體附近區域中之上述下包覆層之折射率之最大值nmax與最小值nmin之差(nmax-nmin)為0.0001以上。 In the resin optical waveguide of the present invention, it is preferable that a difference (n max -n min ) between the maximum value n max and the minimum value n min of the refractive index of the lower cladding layer in the vicinity of the core is 0.0001 or more. .

於本發明之樹脂光波導中,較佳為,上述芯體中之折射率之最大值n'max與上述芯體附近區域中之上述下包覆層之折射率之最大值nmax之差(n'max-nmax)為0.008~0.02。 In the resin optical waveguide of the present invention, it is preferable that a difference between a maximum value n' max of the refractive index in the core body and a maximum value n max of a refractive index of the lower cladding layer in the vicinity of the core body ( n' max -n max ) is 0.008 to 0.02.

於本發明之樹脂光波導中,較佳為,上述下包覆層之相當於上述芯體露出部之部位中,上述芯體附近區域以外之部位之折射率為上 述芯體附近區域中之上述下包覆層之折射率之最小值nmin以下。 In the resin optical waveguide of the present invention, preferably, in a portion of the lower cladding layer corresponding to the exposed portion of the core, a refractive index of a portion other than the vicinity of the core is the above-mentioned region in the vicinity of the core The minimum value of the refractive index of the lower cladding layer is less than or equal to n min .

於本發明之樹脂光波導中,較佳為,上述下包覆層之厚度為10μm以上。 In the resin optical waveguide of the present invention, it is preferable that the thickness of the lower cladding layer is 10 μm or more.

本發明之樹脂光波導較佳為於波長1310nm及波長1550nm之至少一者下為單模光波導。 The resin optical waveguide of the present invention is preferably a single mode optical waveguide at least one of a wavelength of 1310 nm and a wavelength of 1550 nm.

於本發明之樹脂光波導中,較佳為上述樹脂光波導之芯體尺寸為1~10μm。 In the resin optical waveguide of the present invention, it is preferable that the resin optical waveguide has a core size of 1 to 10 μm.

於本發明之樹脂光波導中,較佳為上述樹脂光波導之芯體包含含有氟之樹脂。 In the resin optical waveguide of the present invention, it is preferable that the core of the resin optical waveguide contains a resin containing fluorine.

又,本發明提供一種樹脂光波導,其特徵在於:其係具備芯體以及折射率低於該芯體之下包覆層及上包覆層者,於上述樹脂光波導之一端側,設置有不存在上包覆層而露出芯體及與該芯體鄰接之下包覆層之芯體露出部,樹脂光波導之光傳輸方向之該芯體露出部之長度為500μm以上,且上述下包覆層中相當於上述芯體露出部之部位具有滿足下述(1)~(3)之芯體附近區域:(1)上述芯體附近區域係自上述芯體之距離為x以內之區域,x為10μm以上且20μm以下;(2)上述芯體附近區域具有如下折射率分佈:與上述芯體之界面側之折射率為高,相對於與該芯體之界面之遠位側之折射率變低;(3)上述芯體附近區域中之上述下包覆層之折射率之最大值nmax與最小值nmin之差(nmax-nmin)為0.001以上。 Moreover, the present invention provides a resin optical waveguide characterized in that it has a core body and a cladding layer having a lower refractive index than the lower cladding layer and the upper cladding layer, and is provided on one end side of the resin optical waveguide. The core body and the core exposed portion of the cladding layer adjacent to the core body are exposed without the upper cladding layer, and the length of the core exposed portion of the resin optical waveguide in the light transmission direction is 500 μm or more, and the above-mentioned under package The portion corresponding to the core exposed portion in the coating layer has a region in the vicinity of the core body satisfying the following (1) to (3): (1) a region in the vicinity of the core body from the core body within a distance of x, x is 10 μm or more and 20 μm or less; (2) the vicinity of the core has a refractive index distribution: a refractive index higher on the interface side with the core, and a refractive index on the far side from the interface with the core (3) The difference (n max -n min ) between the maximum value n max and the minimum value n min of the refractive index of the lower cladding layer in the vicinity of the core is 0.001 or more.

本發明之樹脂光波導較佳為於上述芯體露出部與矽光波導連接。 Preferably, the resin optical waveguide of the present invention is connected to the calender waveguide at the core exposed portion.

本發明之樹脂光波導適宜用於低損失且低成本地連接矽光波導 與樹脂光波導之矽光子介面。 The resin optical waveguide of the present invention is suitable for connecting a quenched waveguide with low loss and low cost The photon interface with the resin optical waveguide.

本發明之樹脂光波導於使用單模光纖之性能評價時之連接損失少,性能評價之可靠性高。 The resin optical waveguide of the present invention has a small connection loss when evaluating the performance of a single-mode optical fiber, and has high reliability in performance evaluation.

10‧‧‧樹脂光波導 10‧‧‧Resin Optical Waveguide

11‧‧‧芯體 11‧‧‧ core

12‧‧‧下包覆層 12‧‧‧Under cladding

13‧‧‧上包覆層 13‧‧‧Upper coating

14‧‧‧芯體露出部 14‧‧‧ Core Exposed

100‧‧‧連接器 100‧‧‧Connector

130‧‧‧光纖 130‧‧‧Fiber

140‧‧‧芯體 140‧‧‧ core

200‧‧‧矽光波導晶片 200‧‧‧Lightguide waveguide chip

210‧‧‧矽光波導 210‧‧‧矽光光

220‧‧‧芯體 220‧‧‧ core

230‧‧‧被覆 230‧‧‧covered

300‧‧‧樹脂光波導晶片 300‧‧‧Resin Optical Waveguide Wafer

310‧‧‧樹脂光波導 310‧‧‧Resin Optical Waveguide

320‧‧‧芯體 320‧‧‧ core

330‧‧‧下包覆層 330‧‧‧Under cladding

340‧‧‧上包覆層 340‧‧‧Upper coating

350‧‧‧芯體露出部 350‧‧‧ core body

400‧‧‧單模光纖 400‧‧‧ single mode fiber

410‧‧‧芯體 410‧‧‧ core

420‧‧‧包覆層 420‧‧ ‧ coating

圖1係表示本發明之樹脂光波導之一構成例之立體圖。 Fig. 1 is a perspective view showing a configuration example of a resin optical waveguide of the present invention.

圖2係表示實施例中之樹脂光波導與單模光纖之連接部之模式圖。 Fig. 2 is a schematic view showing a connection portion between a resin optical waveguide and a single mode optical fiber in the embodiment.

圖3係表示矽光子介面之一構成例之立體圖。 Fig. 3 is a perspective view showing a configuration example of a photon interface.

圖4係圖3之矽光子介面之側視圖。 Figure 4 is a side view of the photonic interface of Figure 3.

圖5係表示用於圖3、4之矽光子介面之樹脂光波導之一構成例之立體圖。 Fig. 5 is a perspective view showing a configuration example of a resin optical waveguide used for the photon interface of Figs. 3 and 4.

圖6係表示於圖3、4所示之矽光子介面中形成於矽光波導晶片200上之矽光波導與樹脂光波導310之連接部之剖視圖。 Fig. 6 is a cross-sectional view showing a connection portion between the pupil waveguide and the resin optical waveguide 310 formed on the 波导-waveguide wafer 200 in the 矽 photonic interface shown in Figs.

圖7係用以說明圖3、4所示之矽光子介面中之光之傳輸之模式圖。 Figure 7 is a schematic view for explaining the transmission of light in the photonic interface shown in Figures 3 and 4.

圖8係用以說明於圖5所示之樹脂光波導310之前端連接有單模光纖時之光之傳播之模式圖。 Fig. 8 is a schematic view for explaining the propagation of light when a single mode fiber is connected to the front end of the resin optical waveguide 310 shown in Fig. 5.

以下,參照圖式說明本發明。 Hereinafter, the present invention will be described with reference to the drawings.

圖1係表示本發明之樹脂光波導之一構成例之立體圖。圖1所示之樹脂光波導10具備芯體11以及折射率低於該芯體11之下包覆層12及上包覆層13。於芯體11之下方配置有下包覆層12,於芯體11之上方配置有上包覆層13。但是,於樹脂光波導10之一端側設置有不存在上包覆層13而露出芯體11之芯體露出部14。 Fig. 1 is a perspective view showing a configuration example of a resin optical waveguide of the present invention. The resin optical waveguide 10 shown in FIG. 1 is provided with a core 11 and a cladding layer 12 and an upper cladding layer 13 having a lower refractive index than the core 11. A lower cladding layer 12 is disposed below the core 11 , and an upper cladding layer 13 is disposed above the core 11 . However, the core exposed portion 14 in which the upper cladding layer 13 is absent and the core 11 is exposed is provided on one end side of the resin optical waveguide 10.

再者,於本發明之樹脂光波導中,將配置於芯體周圍之下包覆層及上包覆層中不存在於芯體露出部之側作為上包覆層。因此,亦可 於芯體之上方配置下包覆層,於芯體之下方配置上包覆層。 Further, in the resin optical waveguide of the present invention, the side of the cladding layer and the upper cladding layer which are disposed under the core is not present on the exposed portion of the core as the upper cladding layer. Therefore, it can also The lower cladding layer is disposed above the core body, and the upper cladding layer is disposed under the core body.

該芯體露出部14成為將樹脂光波導10用作矽光子介面時與矽光波導之連接部位。因此,要求芯體露出部14具有足夠用作與矽光波導之連接部位的長度。本發明之樹脂光波導10較佳為樹脂光波導之光傳輸方向之芯體露出部14之長度為100μm以上,其係足夠用作與矽光波導之連接部位的長度。再者,所謂樹脂光波導之光傳輸方向係指芯體11之長軸方向。 The core exposed portion 14 serves as a connection portion with the pupil waveguide when the resin optical waveguide 10 is used as a photonic interface. Therefore, the core exposed portion 14 is required to have a length sufficient to serve as a connection portion with the calender waveguide. The resin optical waveguide 10 of the present invention preferably has a length of the core exposed portion 14 in the light transmission direction of the resin optical waveguide of 100 μm or more, which is sufficient for the length of the connection portion with the calender waveguide. In addition, the light transmission direction of the resin optical waveguide refers to the long axis direction of the core 11.

芯體露出部14之樹脂光波導之光傳輸方向之長度更佳為300μm以上,進而較佳為500μm以上,進而更佳為1000μm以上。 The length of the resin optical waveguide of the core exposed portion 14 in the light transmission direction is more preferably 300 μm or more, further preferably 500 μm or more, and still more preferably 1,000 μm or more.

但是,若樹脂光波導之光傳輸方向之芯體露出部14之長度過長,則於使用接著劑(例如環氧樹脂)與矽光波導連接時,有因接著劑之吸收而導致連接損失變大之虞。因此,樹脂光波導之光傳輸方向之芯體露出部14之長度較佳為10000μm以下,更佳為5000μm以下,進而較佳為3000μm以下。 However, if the length of the core exposed portion 14 in the light transmission direction of the resin optical waveguide is too long, when an adhesive (for example, an epoxy resin) is used to connect with the calender waveguide, the connection loss may be changed by absorption of the adhesive. Big one. Therefore, the length of the core exposed portion 14 in the light transmission direction of the resin optical waveguide is preferably 10000 μm or less, more preferably 5,000 μm or less, and still more preferably 3,000 μm or less.

於樹脂光波導10中,下包覆層12及上包覆層13之折射率低於芯體11之原因在於,防止於芯體11中傳播之光向下包覆層12側或上包覆層13側放射。 In the resin optical waveguide 10, the lower cladding layer 12 and the upper cladding layer 13 have a refractive index lower than that of the core 11 because the light propagating in the core 11 is prevented from being coated on the side of the cladding layer 12 or on the upper side. The layer 13 is radiated.

如上所述,如圖8所示,於連接具有芯體露出部之樹脂光波導310與單模光纖400時,於不存在上包覆層340之芯體露出部,成為芯體320露出之狀態。由於樹脂光波導310之性能評價係於芯體露出部存在於空氣中或水中之狀態下實施,故而芯體320之露出面與空氣或水接觸,但空氣或水之折射率小於樹脂光波導310之芯體320之材料或下包覆層330之材料。其結果為,於芯體320中傳輸之光之一部分向下包覆層330側放射,導致產生連接損失。 As described above, when the resin optical waveguide 310 having the core exposed portion and the single-mode optical fiber 400 are connected as shown in FIG. 8, the core exposed portion of the upper cladding layer 340 is not present, and the core 320 is exposed. . Since the performance evaluation of the resin optical waveguide 310 is performed in a state where the exposed portion of the core is present in the air or in water, the exposed surface of the core 320 is in contact with air or water, but the refractive index of the air or water is smaller than that of the resin optical waveguide 310. The material of the core 320 or the material of the lower cladding layer 330. As a result, a portion of the light transmitted in the core 320 is radiated toward the side of the cladding layer 330, resulting in a connection loss.

本發明之樹脂光波導10中,下包覆層12中相當於芯體露出部14之部位具有滿足下述(1)、(2)之芯體附近區域,藉此,抑制與單模光 纖之連接時之連接損失。 In the resin optical waveguide 10 of the present invention, the portion corresponding to the core exposed portion 14 of the lower cladding layer 12 has a region in the vicinity of the core that satisfies the following (1) and (2), thereby suppressing the single-mode light. Connection loss when the fiber is connected.

(1)芯體附近區域係自芯體11之距離為x以內之區域,x為5μm以上且20μm以下。 (1) The region in the vicinity of the core is a region in which the distance from the core 11 is within x, and x is 5 μm or more and 20 μm or less.

(2)芯體附近區域具有如下折射率分佈:與芯體11之界面側之折射率較高,相對於與該芯體11之界面之遠位側之折射率變低。 (2) The vicinity of the core has a refractive index distribution in which the refractive index on the interface side with the core 11 is higher, and the refractive index on the far side from the interface with the core 11 becomes lower.

藉由於芯體附近區域設置芯體11近位側之折射率較高、芯體11遠位側之折射率變低之折射率分佈,從而,於芯體露出部14,可抑制於芯體11中傳輸之光向下包覆層12側放射,可抑制與單模光纖之連接時之連接損失。再者,上述(2)中之折射率分佈係藉由自與芯體11之界面側朝向相對於與該芯體11之界面之遠位側而折射率連續地變低而產生。 By providing a refractive index distribution in which the refractive index on the proximal side of the core 11 is higher and the refractive index on the distal side of the core 11 is lower in the vicinity of the core, the core exposed portion 14 can be suppressed to the core 11 The transmitted light is radiated to the side of the cladding layer 12, and the connection loss at the time of connection with the single mode fiber can be suppressed. Further, the refractive index distribution in the above (2) is generated by continuously decreasing the refractive index from the interface side with the core 11 toward the distal side with respect to the interface with the core 11.

此處,將芯體附近區域設為自芯體11之距離為x以內之區域,x設為5μm以上,藉此,於芯體露出部14,抑制於芯體11中傳輸之光向下包覆層12側放射。再者,將x之上限設為20μm之原因在於,即便於自芯體11之距離為20μm以上之區域設置上述折射率分佈,對抑制與上述單模光纖之連接時之連接損失之效果之幫助亦較少。 Here, the region in the vicinity of the core is a region in which the distance from the core 11 is within x, and x is set to 5 μm or more, whereby the light emitted from the core 11 is suppressed from being discharged to the core exposed portion 14. The coating 12 is radiated on the side. In addition, the reason why the upper limit of x is 20 μm is that the refractive index distribution is provided in a region where the distance from the core 11 is 20 μm or more, and the effect of suppressing the connection loss when connecting to the single-mode optical fiber is facilitated. Also less.

於本發明之樹脂光波導10中,就抑制與上述單模光纖之連接時之連接損失之效果之方面而言,較佳為芯體附近區域之折射率分佈為0.00004/μm以上。 In the resin optical waveguide 10 of the present invention, in terms of the effect of suppressing the connection loss when the single-mode optical fiber is connected, the refractive index distribution in the vicinity of the core is preferably 0.00004 / μm or more.

芯體附近區域之折射率分佈較佳為0.00007/μm以上,更佳為0.000075/μm以上,進而較佳為0.0001/μm以上,尤佳為0.0002/μm以上。 The refractive index distribution in the vicinity of the core is preferably 0.0007 / μm or more, more preferably 0.000075 / μm or more, further preferably 0.0001 / μm or more, and particularly preferably 0.0002 / μm or more.

再者,折射率分佈之上限值並無特別限定,例如因下述製造方法等而可設為0.00035。 In addition, the upper limit of the refractive index distribution is not particularly limited, and may be, for example, 0.00035 by the following production method or the like.

關於芯體附近區域中之下包覆層12之折射率,相對於芯體11之近位側之折射率成為最大值nmax,相對於芯體11之遠位側之折射率成為 最小值nmin。就抑制與單模光纖之連接時之連接損失之方面而言,芯體附近區域中之下包覆層12之折射率之最大值nmax與最小值nmin之差(nmax-nmin)較佳為0.0001以上,更佳為0.0002以上,進而較佳為0.0004以上,尤佳為0.0008以上。 Regarding the refractive index of the lower cladding layer 12 in the vicinity of the core, the refractive index with respect to the proximal side of the core 11 becomes the maximum value n max , and the refractive index with respect to the far side of the core 11 becomes the minimum value n Min . The difference between the maximum value of the refractive index n max of the lower cladding layer 12 in the vicinity of the core and the minimum value n min (n max -n min ) in terms of the connection loss when the connection to the single mode fiber is suppressed. It is preferably 0.0001 or more, more preferably 0.0002 or more, still more preferably 0.0004 or more, and still more preferably 0.0008 or more.

再者,折射率之最大值nmax與最小值nmin之差之上限值並無特別限定,例如因下述製造方法等而可設為0.0035。 In addition, the upper limit of the difference between the maximum value n max of the refractive index and the minimum value n min is not particularly limited, and may be, for example, 0.0035 by the following production method or the like.

就兼顧抑制與矽光波導之連接損失、及抑制與單模光纖之連接時之連接損失之方面而言,芯體11中之折射率之最大值n'max與芯體附近區域中之下包覆層12之折射率之最大值nmax之差(n'max-nmax)較佳為0.008~0.02。此處,設為芯體11中之折射率之最大值n'max之原因在於,考慮到於芯體11亦存在折射率分佈之情形。 The maximum value of the refractive index n' max in the core 11 and the lower portion in the vicinity of the core are considered in terms of suppressing the connection loss with the boring waveguide and suppressing the connection loss when connecting to the single mode fiber. the difference between the maximum value n max (n 'max -n max) of the refractive index of the cladding layer 12 is preferably 0.008 to 0.02. Here, n is set to the maximum value of the refractive index of the core 11 in the 'max in that reason, in consideration of the refractive index profile of the core of the case 11 is also present.

n'max-nmax更佳為0.010~0.015。 More preferably, n' max -n max is 0.010 to 0.015.

於本發明之樹脂光波導中,就抑制與單模光纖之連接時之連接損失之方面而言,較佳為下包覆層12之相當於芯體露出部之部位中芯體附近區域以外之部位之折射率為芯體附近區域中之下包覆層12之折射率之最小值nmin以下。該芯體附近區域以外之下包覆層12之折射率只要為最小值nmin以下,則無特別限定。因此,上述芯體附近區域以外之部位之折射率可為全部相同之數值,亦可與芯體附近區域之情形同樣地具有朝向相對於芯體11之遠位側而折射率進一步變低之折射率分佈。 In the resin optical waveguide of the present invention, in terms of suppressing the connection loss at the time of connection with the single-mode optical fiber, it is preferable that the portion of the lower cladding layer 12 corresponding to the vicinity of the core in the portion corresponding to the exposed portion of the core is parts of the refractive index of the core region near the body under cladding layer refractive index n min of the minimum value of 12 or less. The refractive index of the coating layer 12 other than the region in the vicinity of the core is not particularly limited as long as it is equal to or less than the minimum value n min . Therefore, the refractive index of the portion other than the region in the vicinity of the core may be all the same value, and may have a refractive index which is further lowered toward the far side with respect to the core 11 as in the case of the vicinity of the core. Rate distribution.

又,於本發明之樹脂光波導中,根據下包覆層12之厚度,下包覆層12之相當於芯體露出部之部位整體亦可為滿足上述(1)、(2)、較佳為滿足上述(1)~(3)之芯體附近區域。於此情形時,下包覆層12之厚度與上述x一致。 Further, in the resin optical waveguide of the present invention, depending on the thickness of the lower cladding layer 12, the entire portion of the lower cladding layer 12 corresponding to the exposed portion of the core may satisfy the above (1), (2), preferably. In order to satisfy the area near the core of the above (1) to (3). In this case, the thickness of the lower cladding layer 12 coincides with the above x.

又,於本發明之樹脂光波導中,關於在芯體11之上下配置有上包覆層13及下包覆層12的部位之下包覆層12之折射率,只要包含芯體附 近區域在內之所有區域均為低於芯體11之折射率之數值,則無特別限定。因此,例如關於該部位之下包覆層12,折射率可為全部相同之數值,亦可具有朝向相對於芯體11之遠位側而折射率變低之折射率分佈。又,亦可具有與滿足上述(1)~(3)之芯體附近區域相同之區域。 Further, in the resin optical waveguide of the present invention, the refractive index of the cladding layer 12 under the portion where the upper cladding layer 13 and the lower cladding layer 12 are disposed above and below the core 11 is included as long as the core is attached. The area including the near region is a value lower than the refractive index of the core 11, and is not particularly limited. Therefore, for example, regarding the cladding layer 12 under the portion, the refractive index may be all the same value, or may have a refractive index distribution which is lower toward the far side of the core 11 and lower in refractive index. Further, it may have the same area as the vicinity of the core body satisfying the above (1) to (3).

對本發明之樹脂光波導進一步記載。 The resin optical waveguide of the present invention is further described.

(芯體11) (core 11)

於圖1所示之樹脂光波導10中,芯體11之剖面形狀為矩形,但並不限於此,例如亦可為梯形、圓形、橢圓形。於芯體11之剖面形狀為多邊形之情形時,其角亦可帶有弧度。 In the resin optical waveguide 10 shown in FIG. 1, the cross-sectional shape of the core 11 is rectangular, but is not limited thereto, and may be, for example, a trapezoidal shape, a circular shape, or an elliptical shape. When the cross-sectional shape of the core 11 is a polygon, the angle may be curved.

芯體尺寸並無特別限定,可考慮與光源或受光元件之耦合效率等而適當設計。耦合效率依存於芯體直徑及數值孔徑(NA)。關於例如芯體11之芯體尺寸(如圖1所示之芯體11般芯體11之剖面形狀為矩形之情形時,為該矩形之寬度及高度),若考慮用作矽光子介面時與所要連接之矽光波導之耦合效率,則較佳為1~10μm。更佳為1.5~8μm,進而較佳為2~7μm。此處,矩形之寬度係於高度中央位置上之寬度之長度,矩形之高度係於寬度中央位置上之高度之長度。再者,芯體尺寸亦可沿樹脂光波導之光傳輸方向呈錐狀變化。 The core size is not particularly limited, and may be appropriately designed in consideration of coupling efficiency with a light source or a light receiving element. The coupling efficiency depends on the core diameter and numerical aperture (NA). Regarding, for example, the core size of the core 11 (when the cross-sectional shape of the core 11 is a rectangle as shown in FIG. 1 , the width and height of the rectangle), when considering the use as a photonic interface, The coupling efficiency of the optical waveguide to be connected is preferably 1 to 10 μm. More preferably, it is 1.5 to 8 μm, and further preferably 2 to 7 μm. Here, the width of the rectangle is the length of the width at the center of the height, and the height of the rectangle is the length of the height at the center of the width. Furthermore, the core size can also be tapered in the direction of light transmission of the resin optical waveguide.

芯體11亦可具有朝向相對於芯體中心之遠位側而折射率變低之折射率分佈。又,可具有上包覆層側之折射率較高而下包覆層側之折射率變低之折射率分佈,亦可具有上包覆層側之折射率較低而下包覆層側之折射率變高之折射率分佈。 The core 11 may also have a refractive index profile that is directed toward the distal side with respect to the center of the core and whose refractive index is lowered. Further, the refractive index distribution having a higher refractive index on the upper cladding layer side and lower refractive index on the lower cladding layer side may have a lower refractive index on the upper cladding layer side and a lower cladding layer side. A refractive index distribution in which the refractive index becomes high.

(上包覆層13) (upper cladding layer 13)

上包覆層13之折射率之數值只要低於芯體11之折射率,則無特別限定。因此,例如上包覆層13可為折射率均為相同之數值,可構成為朝向相對於芯體11之遠位側而折射率變低,亦可構成為朝向相對於芯體11之遠位側而折射率變高。 The numerical value of the refractive index of the upper cladding layer 13 is not particularly limited as long as it is lower than the refractive index of the core 11. Therefore, for example, the upper cladding layer 13 may have a numerical value having the same refractive index, and may be configured such that the refractive index becomes lower toward the distal side with respect to the core 11 or may be configured to face the distal position with respect to the core 11 . The refractive index becomes higher on the side.

上包覆層13之厚度並無特別限定,於本發明之樹脂光波導10為單模光波導之情形時,存在傳輸之光亦洩露至位於距芯體11之中心10μm左右之範圍內之包覆層部分之情況。因此,於單模光波導之情形時,就減少光之傳輸損失之觀點而言,較佳為10μm以上。又,下包覆層12及上包覆層13之合計厚度較佳為20~90μm,更佳為30~70μm。 The thickness of the upper cladding layer 13 is not particularly limited. When the resin optical waveguide 10 of the present invention is a single-mode optical waveguide, the transmitted light is also leaked to a package located within a range of about 10 μm from the center of the core 11. The condition of the cladding part. Therefore, in the case of a single-mode optical waveguide, from the viewpoint of reducing the transmission loss of light, it is preferably 10 μm or more. Further, the total thickness of the lower cladding layer 12 and the upper cladding layer 13 is preferably 20 to 90 μm, more preferably 30 to 70 μm.

於本發明之樹脂光波導中,芯體11、下包覆層12、及上包覆層13之構成材料只要滿足作為樹脂光波導之要求特性,則無特別限定。就抑制於芯體11中傳輸之光之損失之觀點而言,芯體11之構成材料較佳為含有氟之樹脂。 In the resin optical waveguide of the present invention, the constituent materials of the core 11, the lower cladding layer 12, and the upper cladding layer 13 are not particularly limited as long as they satisfy the required characteristics as a resin optical waveguide. The constituent material of the core 11 is preferably a resin containing fluorine, from the viewpoint of suppressing the loss of light transmitted in the core 11.

又,關於芯體11、下包覆層12及上包覆層13之構成材料、以及樹脂光波導之製造程序,例如可參考下述文獻之記載。 Further, the constituent materials of the core 11, the lower cladding layer 12, and the upper cladding layer 13, and the manufacturing procedure of the resin optical waveguide can be referred to, for example, the following documents.

國際公開第2010/107005號 International Publication No. 2010/107005

日本專利特開2013-120338號公報 Japanese Patent Laid-Open Publication No. 2013-120338

日本專利特開2012-63620號公報 Japanese Patent Laid-Open No. 2012-63620

以上述文獻作為參考,製造圖1所示之本發明之樹脂光波導10之情形時,樹脂光波導10之芯體露出部14可按照以下程序形成。 When the resin optical waveguide 10 of the present invention shown in Fig. 1 is produced as a reference, the core exposed portion 14 of the resin optical waveguide 10 can be formed by the following procedure.

形成下包覆層,使用光微影製程於下包覆層上形成芯體後,於下包覆層及芯體上塗佈硬化物組合物,藉由加熱及/或光照射使硬化性樹脂組合物硬化,形成上包覆層。於形成上包覆層時,使用光微影製程,可形成具有上包覆層之區域及無上包覆層而露出芯體之區域(即芯體露出部)。 Forming a lower cladding layer, forming a core on the lower cladding layer by a photolithography process, applying a cured composition on the lower cladding layer and the core, and curing the resin by heating and/or light irradiation The composition hardens to form an upper coating. When the upper cladding layer is formed, a region having the upper cladding layer and a region where the upper cladding layer is absent to expose the core (i.e., the core exposed portion) can be formed by using a photolithography process.

又,具有滿足上述(1)、(2)之芯體附近區域之下包覆層12可按照以下程序形成。 Further, the coating layer 12 having a region in the vicinity of the core body satisfying the above (1) and (2) can be formed by the following procedure.

藉由調整形成上述下包覆層時之加熱溫度或加熱時間,及/或藉由調整光之照射強度或照射時間,可形成具有滿足上述(1)、(2)、較 佳為滿足上述(1)~(3)之芯體附近區域之下包覆層12。或者,藉由添加用以調整折射率之摻雜劑而加以調整,及/或藉由調整光之照射強度或照射時間,可形成具有滿足上述(1)、(2)、較佳為滿足上述(1)~(3)之芯體附近區域之下包覆層12。 By adjusting the heating temperature or heating time when forming the lower cladding layer, and/or by adjusting the irradiation intensity or the irradiation time of the light, it is possible to form the above (1), (2), and It is preferable to satisfy the cladding layer 12 under the vicinity of the core of the above (1) to (3). Alternatively, it may be adjusted by adding a dopant for adjusting the refractive index, and/or by adjusting the irradiation intensity or the irradiation time of the light, and satisfying the above (1), (2), preferably satisfying the above The cladding layer 12 is under the region near the core of (1) to (3).

再者,於藉由添加摻雜劑而調整折射率之情形時,該折射率依存於構成下包覆層之材料及摻雜劑之種類,因此為了獲得目標之折射率,根據構成下包覆層之材料而適當選擇該摻雜劑。 Further, when the refractive index is adjusted by adding a dopant, the refractive index depends on the type of the material constituting the lower cladding layer and the type of the dopant, and therefore, in order to obtain the target refractive index, the under cladding is formed according to the composition. The dopant is appropriately selected from the material of the layer.

本發明之樹脂光波導係被用於低損失且低成本地連接矽光波導與光纖之矽光子介面,因此為單模光波導可使光信號高密度化,故而較佳。於此情形時,於波長1310nm及1550nm之至少一者下為單模光波導時,即便對於矽光波導或單模光纖亦可低損失地傳輸光,故而較佳。 Since the resin optical waveguide of the present invention is used for connecting the photonic interface of the optical waveguide and the optical fiber with low loss and low cost, it is preferable that the optical signal is made denser by the single-mode optical waveguide. In this case, when the single mode optical waveguide is used for at least one of the wavelengths of 1310 nm and 1550 nm, light can be transmitted with low loss even for the neon waveguide or the single mode fiber, which is preferable.

於將本發明之樹脂光波導用於矽光子介面之情形時,於樹脂光波導之芯體露出部與矽光波導連接。 When the resin optical waveguide of the present invention is used for a photonic interface, the core exposed portion of the resin optical waveguide is connected to the calender waveguide.

[實施例] [Examples]

以下使用實施例進一步詳細地說明本發明,但本發明並不限定於該等實施例。 Hereinafter, the present invention will be described in further detail by way of examples, but the invention is not limited to the examples.

於以下所示之實施例中,以RSoft Design Group股份有限公司製造之RSoft CAD定義樹脂光波導與單模光纖之構造(尺寸與折射率),藉由作為模擬‧引擎之RSoft Design Group股份有限公司製造之BeamProp(有限差分光束傳輸法)進行光傳輸之模擬。 In the examples shown below, RSoft CAD, manufactured by RSoft Design Group, Inc., defines the construction (size and refractive index) of resin optical waveguides and single-mode fibers, by RSoft Design Group, Inc., which simulates the ‧ engine The manufactured BeamProp (Finite Differential Beam Transfer Method) performs simulation of optical transmission.

圖2係表示實施例中之樹脂光波導與單模光纖之連接部之模式圖。 Fig. 2 is a schematic view showing a connection portion between a resin optical waveguide and a single mode optical fiber in the embodiment.

(例1~52) (Examples 1~52)

例1~52中,例1~5、7~11、例13~52為實施例,例6、例12為比較例。 In Examples 1 to 52, Examples 1 to 5, 7 to 11, and Examples 13 to 52 are examples, and Examples 6 and 12 are comparative examples.

如以下所示,以RSoft CAD定義樹脂光波導與單模光纖之構造。 The structure of the resin optical waveguide and the single mode fiber is defined by RSoft CAD as shown below.

(單模光纖400) (single mode fiber 400)

芯體410 Core 410

芯體直徑8.4μm Core diameter 8.4μm

折射率1.47 Refractive index 1.47

包覆層420 Coating layer 420

包覆層直徑80μm Coating diameter 80μm

折射率1.4652 Refractive index 1.4652

(樹脂光波導10) (Resin Optical Waveguide 10)

單模光波導 Single mode optical waveguide

芯體11 Core 11

芯體尺寸 寬度方向5.9μm,縱向2.3μm Core size 5.9μm in width direction and 2.3μm in length

折射率1.534 Refractive index 1.534

下包覆層12 Lower cladding layer 12

厚度40μm Thickness 40μm

與芯體11之界面之折射率1.52 The refractive index of the interface with the core 11 is 1.52

於自芯體11之距離為10μm以內之芯體附近區域,具有與芯體11之界面側之折射率較高、相對於與芯體11之界面之遠位側之折射率變低之折射率分佈(0×10-4~3.5×10-4/μm)。 The region in the vicinity of the core within 10 μm from the core 11 has a refractive index higher on the interface side with the core 11 and a lower refractive index on the far side of the interface with the core 11 Distribution (0 × 10 -4 ~ 3.5 × 10 -4 / μm).

上包覆層13 Upper cladding layer 13

厚度40μm Thickness 40μm

折射率1.52 Refractive index 1.52

芯體露出部14 Core exposed portion 14

關於將芯體露出部14以水(折射率1.32)或空氣(折射率1.00)填滿之狀態,根據BeamProp藉由計算求出波長1.55μm下之連接損失。將結果示於下述表。再者,表中,下包覆層12之折射率中,將與芯體11之 界面側之折射率設為n2,將自與芯體11之界面之距離為10μm之位置上之折射率設為n1。再者,n2為芯體附近區域中之下包覆層12之折射率之最大值nmax,n1為芯體附近區域中之下包覆層12之折射率之最小值nmin,又,光波導10之芯體11與單模光纖400之芯體410之偏移量Y如圖2所示。又,表中之指標如下述表所示。 Regarding the state in which the core exposed portion 14 is filled with water (refractive index of 1.32) or air (refractive index of 1.00), the connection loss at a wavelength of 1.55 μm is calculated by BeamProp. The results are shown in the following table. Further, in the table, among the refractive indices of the lower cladding layer 12, the refractive index at the interface side with the core 11 is set to n2, and the refractive index at a position of 10 μm from the interface with the core 11 is set. Is n1. Furthermore, n2 is the maximum value of the refractive index n max of the lower cladding layer 12 in the vicinity of the core, and n1 is the minimum value of the refractive index of the lower cladding layer 12 in the vicinity of the core n min . The offset Y of the core 11 of the waveguide 10 and the core 410 of the single mode fiber 400 is as shown in FIG. Also, the indicators in the table are as shown in the following table.

上述表1~表6係將芯體露出部14之光傳輸方向之長度設為2000μm之實施例,於表7及表8中表示將芯體露出部14之長度設為500μm、1000μm、1500μm及3000μm者之結果。 Tables 1 to 6 are examples in which the length of the core exposed portion 14 in the light transmission direction is 2000 μm, and Tables 7 and 8 show that the length of the core exposed portion 14 is 500 μm, 1000 μm, 1500 μm, and The result of 3000μm.

由表可知,相當於芯體露出部之芯體附近區域不具有折射率分佈之例6、12之連接損失較大。相對於此,相當於芯體露出部之芯體附近區域之折射率分佈為0.00004μm以上之例1~5、例7~11、例13~例52之連接損失較小。 As can be seen from the table, the connection loss of Examples 6 and 12 in which the region near the core of the core exposed portion does not have a refractive index distribution is large. On the other hand, the connection loss of Examples 1 to 5, Examples 7 to 11, and Examples 13 to 52, which correspond to the refractive index distribution in the vicinity of the core of the core exposed portion, is 0.00004 μm or more.

又,如表4~6所示,於將芯體露出部14以水填滿之狀態、或以空氣填滿之狀態之任一情形時,只要芯體附近區域之折射率分佈為0.00004μm以上,則無關於折射率分佈之大小如何,又,因光波導10之芯體14與單模光纖400之芯體410之偏移量Y所導致之影響較少。 Further, as shown in Tables 4 to 6, in the case where the core exposed portion 14 is filled with water or filled with air, the refractive index distribution in the vicinity of the core is 0.00004 μm or more. That is, regardless of the magnitude of the refractive index distribution, and the influence of the offset Y of the core 14 of the optical waveguide 10 and the core 410 of the single mode fiber 400 is less.

(例53、例54) (Example 53, Example 54)

例53為實施例,例54為比較例。作為例53,製作芯體之折射率 為1.53且芯體寬度為6.0μm,芯體高度為2.49μm,上包覆層之厚度為24μm,下包覆層之厚度為50μm之樹脂光波導。下包覆層之芯體界面側之折射率為1.516,且具有隨著自芯體之界面離開而折射率變低之折射率分佈0.00008/μm。關於下包覆層之折射率分佈,具有上包覆層之區域與不具有上包覆層之區域均具有相同之折射率分佈。芯體露出部14之光傳輸方向之長度為1750μm,芯體露出部之狀態為水。該實施例53之樹脂光波導與單模光纖之連接損失為7.0dB,連接損失之指標為「4」。 Example 53 is an example, and Example 54 is a comparative example. As Example 53, the refractive index of the core was made The resin optical waveguide was 1.53 and the core width was 6.0 μm, the core height was 2.49 μm, the thickness of the upper cladding layer was 24 μm, and the thickness of the lower cladding layer was 50 μm. The core layer side of the lower cladding layer has a refractive index of 1.516 and a refractive index distribution of 0.00008/μm which decreases in refractive index as it leaves the interface of the core. Regarding the refractive index distribution of the lower cladding layer, the region having the upper cladding layer and the region having no upper cladding layer have the same refractive index distribution. The length of the core exposed portion 14 in the light transmission direction was 1750 μm, and the state of the exposed portion of the core was water. The connection loss of the resin optical waveguide and the single mode fiber of Example 53 was 7.0 dB, and the connection loss index was "4".

作為例54,下包覆層之折射率遍及厚度方向地設為固定,除此以外,製作與實施例53相同之構造之光纖。下包覆層之折射率固定為1.516。該例54之樹脂光波導與單模光纖之連接損失超過20dB,連接損失之指標為「1」。 In Example 54, an optical fiber having the same structure as that of Example 53 was produced except that the refractive index of the lower cladding layer was fixed throughout the thickness direction. The refractive index of the lower cladding layer was fixed at 1.516. The connection loss of the resin optical waveguide of this example 54 to the single mode fiber exceeded 20 dB, and the connection loss index was "1".

已詳細地且參照特定之實施態樣對本發明進行了說明,但業者明白,可不脫離本發明之精神及範圍而添加各種變更或修正。本申請案係基於2015年8月4日提出申請之日本專利申請案(日本專利特願2015-154011號)者,其內容作為參照引入本文。 The present invention has been described in detail with reference to the specific embodiments thereof, and it is understood that various changes and modifications may be made without departing from the spirit and scope of the invention. The present application is based on Japanese Patent Application No. 2015-154011, filed on Jan.

Claims (11)

一種樹脂光波導,其特徵在於:其係具備芯體以及折射率低於該芯體之下包覆層及上包覆層者,於上述樹脂光波導之一端側,設置有不存在上包覆層而露出芯體及與該芯體鄰接之下包覆層之芯體露出部,且上述下包覆層中相當於上述芯體露出部之部位具有滿足下述(1)、(2)之芯體附近區域:(1)上述芯體附近區域係自上述芯體之距離為x以內之區域,該x為5μm以上且20μm以下;(2)上述芯體附近區域具有如下折射率分佈:與上述芯體之界面側之折射率為高,相對於與該芯體之界面之遠位側之折射率變低。 A resin optical waveguide characterized in that it has a core body and a refractive index lower than a cladding layer and an upper cladding layer of the core body, and is provided on one end side of the resin optical waveguide The core body and the core exposed portion of the cladding layer adjacent to the core body are exposed, and the portion corresponding to the core exposed portion of the lower cladding layer satisfies the following (1) and (2). The region in the vicinity of the core: (1) the region in the vicinity of the core is a region within a distance of x from the core, and x is 5 μm or more and 20 μm or less; (2) the region near the core has the following refractive index distribution: The refractive index of the interface side of the core is high, and the refractive index with respect to the far side of the interface with the core becomes low. 如請求項1之樹脂光波導,其中上述芯體露出部之光傳輸方向之長度為100μm以上。 The resin optical waveguide according to claim 1, wherein the length of the core exposed portion in the light transmission direction is 100 μm or more. 如請求項1或2之樹脂光波導,其中上述芯體附近區域之折射率分佈為0.00004/μm以上。 The resin optical waveguide according to claim 1 or 2, wherein a refractive index distribution of a region in the vicinity of the core is 0.00004 / μm or more. 如請求項1至3中任一項之樹脂光波導,其中上述芯體附近區域中之上述下包覆層之折射率之最大值nmax與最小值nmin之差(nmax-nmin)為0.0001以上。 The resin optical waveguide according to any one of claims 1 to 3, wherein a difference between a maximum value n max of a refractive index of the lower cladding layer in the vicinity of the core body and a minimum value n min (n max -n min ) It is 0.0001 or more. 如請求項1至4中任一項之樹脂光波導,其中上述芯體中之折射率之最大值n'max與上述芯體附近區域中之上述下包覆層之折射率之最大值nmax之差(n'max-nmax)為0.008~0.02。 The resin optical waveguide according to any one of claims 1 to 4, wherein a maximum value of the refractive index n'max in the core and a maximum value of a refractive index of the lower cladding layer in the vicinity of the core are n max The difference (n' max -n max ) is 0.008 to 0.02. 如請求項1至5中任一項之樹脂光波導,其中上述下包覆層之相當於上述芯體露出部之部位中,上述芯體附近區域以外之部位之折射率為上述芯體附近區域中之上述下包覆層之折射率之最 小值nmin以下。 The resin optical waveguide according to any one of claims 1 to 5, wherein, in a portion of the lower cladding layer corresponding to the exposed portion of the core, a refractive index of a portion other than the vicinity of the core is a region near the core The minimum value of the refractive index of the lower cladding layer is less than or equal to n min . 如請求項1至6中任一項之樹脂光波導,其中上述樹脂光波導於波長1310nm及波長1550nm之至少一者下為單模光波導。 The resin optical waveguide according to any one of claims 1 to 6, wherein the resin optical waveguide is a single mode optical waveguide at at least one of a wavelength of 1310 nm and a wavelength of 1550 nm. 如請求項1至7中任一項之樹脂光波導,其中上述樹脂光波導之芯體尺寸為1~10μm。 The resin optical waveguide according to any one of claims 1 to 7, wherein the resin optical waveguide has a core size of 1 to 10 μm. 如請求項1至8中任一項之樹脂光波導,其中上述樹脂光波導之芯體包含含有氟之樹脂。 The resin optical waveguide according to any one of claims 1 to 8, wherein the core of the resin optical waveguide comprises a resin containing fluorine. 一種樹脂光波導,其特徵在於:其係具備芯體以及折射率低於該芯體之下包覆層及上包覆層者,於上述樹脂光波導之一端側,設置有不存在上包覆層而露出芯體及與該芯體鄰接之下包覆層之芯體露出部,樹脂光波導之光傳輸方向之該芯體露出部之長度為500μm以上,且上述下包覆層中相當於上述芯體露出部之部位具有滿足下述(1)~(3)之芯體附近區域:(1)上述芯體附近區域係自上述芯體之距離為x以內之區域,x為10μm以上且20μm以下;(2)上述芯體附近區域具有如下折射率分佈:與上述芯體之界面側之折射率為高,相對於與該芯體之界面之遠位側之折射率變低;(3)上述芯體附近區域中之上述下包覆層之折射率之最大值nmax與最小值nmin之差(nmax-nmin)為0.001以上。 A resin optical waveguide characterized in that it has a core body and a refractive index lower than a cladding layer and an upper cladding layer of the core body, and is provided on one end side of the resin optical waveguide The core body and the core exposed portion of the cladding layer adjacent to the core body are exposed, and the length of the core exposed portion of the resin optical waveguide in the light transmission direction is 500 μm or more, and the lower cladding layer is equivalent to The portion of the exposed portion of the core has a region in the vicinity of the core that satisfies the following (1) to (3): (1) a region in the vicinity of the core in which the distance from the core is within x, and x is 10 μm or more. 20 μm or less; (2) the region near the core has a refractive index distribution: the refractive index on the interface side with the core is high, and the refractive index on the far side of the interface with the core becomes lower; (3) The difference (n max - n min ) between the maximum value n max and the minimum value n min of the refractive index of the lower cladding layer in the vicinity of the core is 0.001 or more. 如請求項1至10中任一項之樹脂光波導,其係於上述芯體露出部與矽光波導連接。 The resin optical waveguide according to any one of claims 1 to 10, wherein the core exposed portion is connected to the pupil waveguide.
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CA2994519C (en) 2023-08-22
EP3333607A1 (en) 2018-06-13
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CA2994519A1 (en) 2017-02-09
US20180156970A1 (en) 2018-06-07
US10222554B2 (en) 2019-03-05
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WO2017022719A1 (en) 2017-02-09
TWI693435B (en) 2020-05-11

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